Measurement of the Z→ττ cross section with the ATLAS detector
The Z→ττ cross section is measured with the ATLAS experiment at the LHC in four different final states determined by the decay modes of the τ leptons: muon-hadron, electron-hadron, electron-muon, and muon-muon. The analysis is based on a data sample corresponding to an integrated luminosity of 36pb...
Guardado en:
Autor principal: | |
---|---|
Formato: | JOUR |
Acceso en línea: | http://hdl.handle.net/20.500.12110/paper_15507998_v84_n11_p_Aad |
Aporte de: |
id |
todo:paper_15507998_v84_n11_p_Aad |
---|---|
record_format |
dspace |
spelling |
todo:paper_15507998_v84_n11_p_Aad2023-10-03T16:24:29Z Measurement of the Z→ττ cross section with the ATLAS detector Aad, G. The Z→ττ cross section is measured with the ATLAS experiment at the LHC in four different final states determined by the decay modes of the τ leptons: muon-hadron, electron-hadron, electron-muon, and muon-muon. The analysis is based on a data sample corresponding to an integrated luminosity of 36pb - 1, at a proton-proton center-of-mass energy of √s=7TeV. Cross sections are measured separately for each final state in fiducial regions of high detector acceptance, as well as in the full phase space, over the mass region 66-116 GeV. The individual cross sections are combined and the product of the total Z production cross section and Z→ττ branching fraction is measured to be 0.97±0.07(stat)±0.06(syst)±0.03(lumi)nb, in agreement with next-to-next-to-leading order calculations. © 2011 CERN. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_15507998_v84_n11_p_Aad |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
repository_str |
R-134 |
collection |
Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
The Z→ττ cross section is measured with the ATLAS experiment at the LHC in four different final states determined by the decay modes of the τ leptons: muon-hadron, electron-hadron, electron-muon, and muon-muon. The analysis is based on a data sample corresponding to an integrated luminosity of 36pb - 1, at a proton-proton center-of-mass energy of √s=7TeV. Cross sections are measured separately for each final state in fiducial regions of high detector acceptance, as well as in the full phase space, over the mass region 66-116 GeV. The individual cross sections are combined and the product of the total Z production cross section and Z→ττ branching fraction is measured to be 0.97±0.07(stat)±0.06(syst)±0.03(lumi)nb, in agreement with next-to-next-to-leading order calculations. © 2011 CERN. |
format |
JOUR |
author |
Aad, G. |
spellingShingle |
Aad, G. Measurement of the Z→ττ cross section with the ATLAS detector |
author_facet |
Aad, G. |
author_sort |
Aad, G. |
title |
Measurement of the Z→ττ cross section with the ATLAS detector |
title_short |
Measurement of the Z→ττ cross section with the ATLAS detector |
title_full |
Measurement of the Z→ττ cross section with the ATLAS detector |
title_fullStr |
Measurement of the Z→ττ cross section with the ATLAS detector |
title_full_unstemmed |
Measurement of the Z→ττ cross section with the ATLAS detector |
title_sort |
measurement of the z→ττ cross section with the atlas detector |
url |
http://hdl.handle.net/20.500.12110/paper_15507998_v84_n11_p_Aad |
work_keys_str_mv |
AT aadg measurementofthezttcrosssectionwiththeatlasdetector |
_version_ |
1807324083485933568 |